Method and system of reducing charged particle beam write time

ABSTRACT

A method for exposing a pattern in an area on a surface using a charged particle beam lithography is disclosed and includes inputting an original set of exposure information for the area. A backscatter is calculated for the area of the pattern based on the exposure information. An artificial background dose is determined for the area. The artificial background dose comprises additional exposure information and is combined with the original set of exposure information creating a modified set of exposure information. A system for exposing a pattern in an area on a surface using a charged particle beam lithography is also disclosed.

BACKGROUND OF THE DISCLOSURE

The present disclosure is related to lithography, and more particularly to the design and manufacture of a surface which may be a reticle, a wafer, or any other surface, using charged particle beam lithography.

Three common types of charged particle beam lithography are unshaped (Gaussian) beam lithography, shaped charged particle beam lithography, and multi-beam lithography. In all types of charged particle beam lithography, charged particle beams shoot energy to a resist-coated surface to expose the resist.

Shaped charged particle beam lithography may be variable shaped beam (VSB) or character projection (CP), in which a shot of a precise electron beam is shaped and steered so as to expose a resist-coated surface, such as the surface of a wafer or the surface of a reticle. In VSB, these shapes are simple shapes, usually limited to rectangles of certain minimum and maximum sizes and with sides which are parallel to the axes of a Cartesian coordinate plane (i.e. of “manhattan” orientation), and 45 degree right triangles (i.e. triangles with their three internal angles being 45 degrees, 45 degrees, and 90 degrees) of certain minimum and maximum sizes. At predetermined locations, doses of electrons are shot into the resist with these simple shapes. The total writing time for this type of system increases with the number of shots. In CP, there is a stencil in the system that has in it a variety of apertures or characters which may be complex shapes such as rectilinear, arbitrary-angled linear, circular, nearly circular, annular, nearly annular, oval, nearly oval, partially circular, partially nearly circular, partially annular, partially nearly annular, partially nearly oval, or arbitrary curvilinear shapes, and which may be a connected set of complex shapes or a group of disjointed sets of a connected set of complex shapes. An electron beam can be shot through a character on the stencil to efficiently produce more complex patterns on the reticle. In theory, such a system can be faster than a VSB system because it can shoot more complex shapes with each time-consuming shot. Thus, an E-shaped pattern shot with a VSB system takes four shots, but the same E-shaped pattern can be shot with one shot with a CP system.

Shaped charged particle beam lithography may use either a single shaped beam, or may use a plurality of shaped beams simultaneously exposing a surface, the plurality of shaped beams producing a higher writing speed than a single shaped beam. When a plurality of charged particle beams simultaneously expose a surface, the charged particle beam lithography is often referred to as a multi-beam lithography. Multi-beam lithography may be multiple beams of shaped or unshaped charged particle beam lithography.

In lithography the lithographic mask or reticle comprises geometric patterns corresponding to the circuit components to be integrated onto a substrate. The patterns used to manufacture the reticle may be generated utilizing computer-aided design (CAD) software or programs. In designing the patterns the CAD program may follow a set of pre-determined design rules in order to create the reticle. These rules are set by processing, design, and end-use limitations. An example of an end-use limitation is defining the geometry of a transistor in a way in which it cannot sufficiently operate at the required supply voltage. In particular, design rules can define the space tolerance between circuit devices or interconnect lines. The design rules are, for example, used to ensure that the circuit devices or lines do not interact with one another in an undesirable manner. For example, the design rules are used so that lines do not get too close to each other in a way that may cause a short circuit. The design rule limitations reflect, among other things, the smallest dimensions that can be reliably fabricated. When referring to these small dimensions, one usually introduces the concept of a critical dimension. These are, for instance, defined as the important widths or areas of a feature or the important space between two features or important space areas, those dimensions requiring exquisite control.

In the production or manufacturing of semiconductor devices, such as integrated circuits, optical lithography may be used to fabricate the semiconductor devices. Optical lithography is a printing process in which a lithographic mask or photomask or reticle is used to transfer patterns to a substrate such as a semiconductor or silicon wafer to create the integrated circuit (I.C.). Other substrates could include flat panel displays, holographic masks or even other reticles. Conventional optical lithography typically uses radiation of 193 nm wavelength or longer. Extreme ultraviolet (EUV) or X-ray lithography are also considered types of optical lithography, but use wavelengths much shorter than the 193 nm of conventional optical lithography. The reticle or multiple reticles may contain a circuit pattern corresponding to an individual layer of the integrated circuit, and this pattern can be imaged onto a certain area on the substrate that has been coated with a layer of radiation-sensitive material known as photoresist or resist. Conventional optical lithography writing machines typically reduce the photomask pattern by a factor of four during the optical lithographic process. Therefore, patterns formed on the reticle or mask must be four times larger than the size of the desired pattern on the substrate or wafer.

In the production or manufacturing of semiconductor devices, such as integrated circuits, non-optical methods may be used to transfer a pattern on a lithographic mask to a substrate such as a silicon wafer. Nanoimprint lithography (NIL) is an example of a non-optical lithography process. In NIL, a lithographic mask pattern is transferred to a substrate through contact of the lithography mask with the substrate. The lithography mask of NIL is typically manufactured as a manufacture of a surface using charged particle beam lithography.

In the production or manufacturing of semiconductor devices, such as integrated circuits, maskless direct write may also be used to fabricate the semiconductor devices. Maskless direct write is a printing process in which charged particle beam lithography is used to transfer patterns to a substrate such as a semiconductor or silicon wafer to create an integrated circuit. Other substrates could include flat panel displays, imprint masks for nano-imprinting, or even reticles. Desired patterns of a layer are written directly on the surface, which in this case is also the substrate. Once the patterned layer is transferred, the layer may undergo various other processes such as etching, ion-implantation (doping), metallization, oxidation, and polishing. These processes are employed to finish an individual layer in the substrate. If several layers are required, then the whole process or variations thereof will be repeated for each new layer. Some of the layers may be written using optical lithography while others may be written using maskless direct write to fabricate the same substrate. Also, some patterns of a given layer may be written using optical lithography, and other patterns written using maskless direct write. Eventually, a combination of multiples of devices or integrated circuits will be present on the substrate. These integrated circuits are then separated from one another by dicing or sawing and then mounted into individual packages. In the more general case, the patterns on the surface may be used to define artifacts such as display pixels, holograms, or magnetic recording heads.

One goal in integrated circuit fabrication by optical lithography is to reproduce the original circuit design on a substrate by use of a reticle, in which the reticle, sometimes referred to as a mask or a photomask, is a surface which may be exposed using charged particle beam lithography. Integrated circuit fabricators are always attempting to use the semiconductor wafer real estate as efficiently as possible. Engineers keep shrinking the size of the circuits to allow the integrated circuits to contain more circuit elements and to use less power. As the size of an integrated circuit critical dimension is reduced and its circuit density increases, the critical dimension of the circuit pattern or physical design approaches the resolution limit of the optical exposure tool used in conventional optical lithography. As the critical dimensions of the circuit pattern become smaller and approach the resolution value of the exposure tool, the accurate transcription of the physical design to the actual circuit pattern developed on the resist layer becomes difficult. To further the use of optical lithography to transfer patterns having features that are smaller than the light wavelength used in the optical lithography process, a process known as optical proximity correction (OPC) has been developed. OPC alters the physical design to compensate for distortions caused by effects such as optical diffraction and the optical interaction of features with proximate features. Resolution enhancement technologies performed with a reticle include OPC and inverse lithography technology (ILT).

OPC may add sub-resolution lithographic features to mask patterns to reduce differences between the original physical design pattern, that is, the design, and the final transferred circuit pattern on the substrate. The sub-resolution lithographic features interact with the original patterns in the physical design and with each other and compensate for proximity effects to improve the final transferred circuit pattern. One feature that is added to improve pattern transference is referred to as “serifs”. Serifs are small features that enhance precision or resiliency to manufacturing variation of printing of a particular feature. An example of a serif is a small feature that is positioned on a corner of a pattern to sharpen the corner in the final transferred image. Patterns that are intended to print on the substrate are referred to as main features. Serifs are a part of a main feature. It is conventional to discuss the OPC-decorated patterns to be written on a reticle in terms of main features, that is features that reflect the design before OPC decoration, and OPC features, where OPC features might include serifs, jogs, sub-resolution assist features (SRAFs) and negative features. OPC features are subject to various design rules, such as a rule based on the size of the smallest feature that can be transferred to the wafer using optical lithography. Other design rules may come from the mask manufacturing process or, if a character projection charged particle beam writing system is used to form the pattern on a reticle, from the stencil manufacturing process.

SRAF features are used to improve the transfer of the pattern. It is often the case that the precision or accuracy demanded of the surface manufacturing process for SRAFs are less than those for main features. There are similar decorations introduced by OPC as negative features. Inside of a large feature, there may be narrow spaces introduced to enhance lithographic performance. Narrow spaces are harder to write reliably than equally narrow lines, so these negative features often end up being the most difficult parts to write reliably on a surface.

SUMMARY OF THE DISCLOSURE

Methods and systems for exposing a pattern in an area on a surface using a charged particle beam lithography include inputting an original set of exposure information for the area. A backscatter is calculated for the area of the pattern based on the exposure information. An artificial background dose is determined for the area. The artificial background dose comprises additional exposure information and is combined with the original set of exposure information creating a modified set of exposure information.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 illustrates an example of a variable shaped beam (VSB) charged particle beam system, as known in the art.

FIG. 2 illustrates an example of an electro-optical schematic diagram of a multi-beam exposure system, as known in the art.

FIGS. 3A-3D illustrate various types of shots, as known in the art.

FIG. 4 illustrates an example of a multi-beam charged particle beam system, as known in the art.

FIGS. 5A-5C and 6A-6C illustrate how dose is affected after PEC for areas with both large and small shapes, as known in the art.

FIGS. 7A-7G illustrate PEC iterations and resulting dosage curves of a rectangular shape, as known in the art.

FIGS. 8A-8F illustrate examples of low-density exposure to high-density exposure, as known in the art.

FIGS. 9A-9B illustrate a low-density exposure area, with artificial background dosage added in accordance with embodiments of the current disclosure.

FIGS. 10A-10F illustrate example embodiments of artificial background dose.

FIG. 11 illustrates a conceptual flow diagram for preparing a surface or reticle for use in fabricating a substrate such as an integrated circuit on a silicon wafer, as known in the art.

FIG. 12 illustrates an example computing hardware device used in embodiments of the methods.

FIG. 13 illustrates a flow in which artificial background dose is calculated, in accordance with some embodiments.

DETAILED DESCRIPTION OF THE EMBODIMENTS

The present disclosure describes methods for reducing charged particle beam write time by reducing the dose required to expose a shot or a shape in a relatively low-density exposure area by casting an artificial background dose in the area.

The cost of charged particle beam lithography is directly related to the time required to expose a pattern on a surface, such as a reticle or wafer. Conventionally, the exposure time is related to the amount of exposure required to write the pattern. For the most complex integrated circuit designs, forming the set of layer patterns, either on a set of reticles or on a substrate, is a costly and time-consuming process. It would therefore be advantageous to be able to reduce the exposure required to form these patterns, on a reticle and other surfaces, such as by reducing the time required to write them.

Referring now to the drawings, wherein like numbers refer to like items, FIG. 1 illustrates an embodiment of a lithography system, such as a charged particle beam writer system, in this case an electron beam writer system 100, that employs a variable shaped beam (VSB) to manufacture a surface 112. The electron beam writer system 100 has an electron beam source 114 that projects an electron beam 116 toward an aperture plate 118. The plate 118 has an aperture 120 formed therein which allows the electron beam 116 to pass. Once the electron beam 116 passes through the aperture 120 it is directed or deflected by a system of lenses (not shown) as electron beam 122 toward another rectangular aperture plate or stencil mask 124. The stencil 124 has formed therein a number of openings or apertures 126 that define various simple shapes such as rectangles and triangles. Each aperture 126 formed in the stencil 124 may be used to form a pattern in the surface 112 of a substrate 134, such as a silicon wafer, a reticle or other substrate. An electron beam 130 emerges from one of the apertures 126 and passes through an electromagnetic or electrostatic reduction lens 138, which reduces the size of the pattern emerging from the aperture 126. In commonly available charged particle beam writer systems, the reduction factor is between 10 and 60. The reduced electron beam 140 emerges from the reduction lens 138 and is directed by a series of deflectors 142 onto the surface 112 as a pattern 128. The surface 112 is coated with resist (not shown) which reacts with the electron beam 140. The electron beam 122 may be directed to overlap a variable portion of an aperture 126, affecting the size and shape of the pattern 128. Blanking plates (not shown) may be used to deflect the beam 116 or the shaped beam 122 so as to prevent the electron beam from reaching the surface 112 during a period after each shot when the lenses directing the beam 122 and the deflectors 142 are being re-adjusted for the succeeding shot. Stencil 124 may in itself act as a deflector by having the beam 116 be deflected to hit unopened portions of the stencil 124. Typically the blanking plates are positioned so as to deflect the electron beam 116 to prevent it from illuminating aperture 120. Conventionally, the blanking period may be a fixed length of time, or it may vary depending, for example, on how much the deflector 142 must be re-adjusted for the position of the succeeding shot. Note that VSB systems can be thought of as a special (simple) case of character projection, where the characters are just simple characters, usually rectangles or 45 degree right triangles. It is also possible to partially expose a character. This can be done by, for instance, blocking part of the particle beam. In this disclosure, partial projection is used to mean both character projection and VSB projection.

In electron beam writer system 100, the substrate 134 is mounted on a movable platform or stage 132. The stage 132 allows substrate 134 to be repositioned so that patterns which are larger than the maximum deflection capability or field size of the charged particle beam 140 may be written to surface 112 in a series of subfields, where each subfield is within the capability of deflector 142 to deflect the beam 140. In one embodiment the substrate 134 may be a reticle. In this embodiment, the reticle, after being exposed with the pattern, undergoes various manufacturing steps through which it becomes a lithographic mask or photomask. The mask may then be used in an optical lithography machine to project an image of the reticle pattern 128, generally reduced in size, onto a silicon wafer to produce an integrated circuit. More generally, the mask is used in another device or machine to transfer the pattern 128 on to a substrate (not illustrated).

The shot dosage of a charged particle beam writer such as an electron beam writer system, whether VSB, CP, or a multi-beam machine, is a function of the intensity of the beam source 114, in this VSB example, and the exposure time for each shot. Typically, the beam intensity remains fixed, and the exposure time is varied to obtain variable shot dosages. The exposure time may be varied to compensate for mid-range effect correction (MEC), various long-range effects such as loading-effect correction (LEC) and fogging-effect correction (FEC) and backscatter in a process called proximity effect correction (PEC). In this disclosure, the term PEC is used to describe MEC, LEC, FEC, and backscatter correction. Electron beam writer systems usually allow setting an overall dosage, called a base dosage, that affects all shots in an exposure pass. Some electron beam writer systems perform dosage compensation calculations within the electron beam writer system itself, and do not allow the dosage of each shot to be assigned individually as part of the input shot list, the input shots therefore having unassigned shot dosages. In such electron beam writer systems all shots have the base dosage, before PEC. Other electron beam writer systems do allow dosage assignment on a shot-by-shot basis. In electron beam writer systems that allow shot-by-shot dosage assignment, the number of available dosage levels may be 64 to 4096 or more, or there may be a relatively few available dosage levels, such as 3 to 8 levels. Some embodiments of the current disclosure are targeted for use with charged particle beam writing systems which allow assignment of dosage levels.

A charged particle beam system may expose a surface with a plurality of individually-controllable beams or beamlets. FIG. 2 illustrates an electro-optical schematic diagram in which there are three charged particle beamlets 210. Associated with each beamlet 210 is a beam controller 220. Each beam controller 220 can, for example, allow its associated beamlet 210 to strike surface 230, and can also prevent beamlet 210 from striking the surface 230. In some embodiments, beam controller 220 may also control beam blur, magnification, size and/or shape of beamlet 210. In this disclosure, a charged particle beam system which has a plurality of individually-controllable beamlets is called a multi-beam system. In some embodiments, charged particles from a single source may be sub-divided to form a plurality of beamlets 210. In other embodiments a plurality of sources may be used to create the plurality of beamlets 210. In some embodiments, beamlets 210 may be shaped by one or more apertures, whereas in other embodiments there may be no apertures to shape the beamlets. Each beam controller 220 may allow the period of exposure of its associated beamlet to be controlled individually. Generally, the beamlets will be reduced in size by one or more lenses (not shown) before striking the surface 230, which will typically be coated with a resist. In some embodiments each beamlet may have a separate electro-optical lens, while in other embodiments a plurality of beamlets, including possibly all beamlets, will share an electro-optical lens.

FIGS. 3A-3D illustrate various types of shots. FIG. 3A illustrates an example of a rectangular shot 310. A VSB charged particle beam system can, for example, form rectangular shots in a variety of x and y dimensions. FIG. 3B illustrates an example of a CP shot 320, which is circular in this example. Any shape can be represented as a CP shot, such as octagons or more complex shapes such as the letter E. For purposes of this disclosure, a shot is an exposure of some surface area over a period of time. The area may be comprised of multiple discontinuous smaller areas. A shot may be comprised of a plurality of other shots which may or may not overlap, and which may or may not be exposed simultaneously. A shot may comprise a specified dose, or the dose may be unspecified. Shots may use a shaped beam, an unshaped beam, or a combination of shaped and unshaped beams.

FIG. 3C illustrates an example of a shot 350 that is an array of circular patterns 352. Shot 350 may be formed in a variety of ways, including multiple shots of a single circular CP character, one or more shots of a CP character which is an array of circular apertures, and one or more multi-beam shots using circular apertures. FIG. 3D illustrates an example of a shot 360 that is a sparse array of rectangular patterns 362 and 364. Shot 360 may be formed in a variety of ways, including a plurality of VSB shots, a CP shot, and one or more multi-beam shots using rectangular apertures. In some embodiments of multi-beam, shot 360 may comprise a plurality of interleaved groups of other multi-beam shots. For example, patterns 362 may be shot simultaneously, then patterns 364 may be shot simultaneously at a time different from patterns 362.

FIG. 4 illustrates an embodiment of a charged particle beam exposure system 400. Charged particle beam system 400 is a multi-beam system, in which a plurality of individually-controllable shaped beams can simultaneously expose a surface. Multi-beam system 400 has an electron beam source 402 that creates an electron beam 404. The electron beam 404 is directed toward aperture plate 408 by condenser 406, which may include electrostatic and/or magnetic elements. Aperture plate 408 has a plurality of apertures 410 which are illuminated by electron beam 404, and through which electron beam 404 passes to form a plurality of shaped beamlets 436. Thus, the multi-beam charged particle beam system 400 comprises the charged particle beam source 402 and aperture plate 408, where the aperture plate 408 comprises a plurality of apertures 410 which the charged particle beam 402 source illuminates. In some embodiments, the multi-beam charged particle beam system comprises a single aperture plate 408. In some embodiments, aperture plate 408 may have hundreds or thousands of apertures 410. Although FIG. 4 illustrates an embodiment with a single electron beam source 402, in other embodiments apertures 410 may be illuminated by electrons from a plurality of electron beam sources. Apertures 410 may be circular, as shown in FIG. 4, or may be of a different shape, for example rectangular aperture 120 as shown in FIG. 1. The set of beamlets 436 then illuminates a blanking controller plate 432. The blanking controller plate 432 has a plurality of blanking controllers 434, each of which is aligned with a beamlet 436. Each blanking controller 434 can individually control its associated beamlet 436, so as to either allow the beamlet 436 to strike surface 424, or to prevent the beamlet 436 from striking the surface 424. The amount of time for which the beam strikes the surface controls the total energy or “dose” applied by that beamlet. Typically, multi-beam writers scan the entire area to be exposed. Therefore, the writing time is constant regardless of shape count or shape complexity.

Substrate 426 is positioned on movable platform or stage 428, which can be repositioned using actuators 430. By moving stage 428, beam 440 can expose an area larger than the dimensions of the maximum size pattern formed by beamlet group 440, using a plurality of exposures or shots. In some embodiments, the stage 428 remains stationary during an exposure, and is then repositioned for a subsequent exposure. In other embodiments, stage 428 moves continuously and at a variable velocity. In yet other embodiments, stage 428 moves continuously but at a constant velocity, which can increase the accuracy of the stage positioning. For those embodiments in which stage 428 moves continuously, a set of deflectors (not shown) may be used to move the beam to match the direction and velocity of stage 428, allowing the beamlet group 440 to remain stationary with respect to surface 424 during an exposure. In still other embodiments of multi-beam systems, individual beamlets in a beamlet group may be deflected across surface 424 independently from other beamlets in the beamlet group.

Other types of multi-beam systems may create a plurality of unshaped beamlets 436, such as by using a plurality of charged particle beam sources to create an array of Gaussian beamlets. While the present disclosure is described in terms of charged particle beam lithography, the methods described may also be applied to laser lithography, particularly to multi-beam laser lithography.

Dose is controlled in all high-precision eBeam writers by controlling the exposure time, rather than by changing the beam's current density dynamically. By practice, it is understood that exposure time can be much more precisely controlled than current density. Because of this, high dose exposure is accomplished by increasing the time that the beam is on compared to low dose exposures. It is conceivable for an eBeam writer to have variable current densities. The present embodiments of this disclosure are applicable if dose control is accomplished at least partially by controlling the exposure time. The exposure time for each beamlet 436 in the beamlet group can be controlled individually using blanking controllers 434. Therefore, multi-beam write time is determined by the maximum dose that needs to be applied. In writers where the stage stops for each beamlet group—for example, a stripe—the highest-dosage beamlet affects the exposure time for the entire stripe. In writers with constant-speed stages, the speed could be constant for the entire design, which may be a subset of a reticle, a full reticle or a wafer or any other surface, or partially constant for a period of time. Therefore, the highest dosage beamlet in a stripe can determine the stage speed and therefore determine the write time for an entire design or surface. Even in variable speed stages, the speed cannot change too quickly as the stage is heavy in order to provide stability, and accelerating or decelerating speed takes a lot of energy and is a source of vibration and blur.

In advanced process nodes, features that need to be precisely written on the mask are less than 3× the size compared to the typical combined blur radius of the forward scattering and resist blur of a typical resist used to print the mask fast enough to be of commercial value. In typical leading edge masks, sub-resolution assist features (SRAFs) of less than 60 nm in width are written on the mask with the combined blur being above 20 nm in range. On masks for EUV lithography, it is generally expected that SRAFs of approximately 30 nm width will become commonly required on masks. In the optical proximity correction (OPC) or inverse lithography technology (ILT) step that produces the mask shapes, wafer performance can be enhanced further if smaller shapes (such as SRAFs) can be printed accurately. But it is also critical that mask shapes produced by OPC/ILT can actually be reliably produced on mask, across mask process variation. Mask design rules, such as minimum allowed feature width and minimum allowed feature spacing on mask, are established that represent the trade-off. OPC/ILT needs to guarantee that the output adheres to the mask design rules. The mask makers need to produce masks that adhere to the mask design rules accurately across manufacturing variation to a certain agreed upon specification. Narrower shapes are more difficult to write on a mask. A small square shape is the most difficult to write. But since small square shapes have smaller impact on wafer performance, typically, a need to write narrow SRAFs accurately is important in leading edge mask processing.

Writing such small shapes on a mask in the presence of other shapes that are larger on the same mask typically is accomplished with dose modulation. Since overall mask write time is one of the principal drivers of mask costs, a resist whose sensitivity is sufficient to achieve the desired accuracy for the larger “main” features is chosen to represent the accuracy-speed/cost trade-off. But writing SRAFs and other smaller shapes also needs to be done accurately, and a common technique is to enhance—i.e., increase—or partially enhance the dose of the SRAFs to cause them to be printed better.

In the industry, the amount by which a normal dose is enhanced can typically vary from 1.2 times the normal dose to 3 times the normal dose, although the dose may be any multiple of normal dose. More enhancement leads to longer write times but can lead to more accurate printing of smaller shapes. FIGS. 5A-5B illustrate the difference between a large enough shape 502 and its dose profile (i.e., dose curve) 512 and a smaller SRAF shape 506 and its dose profile 522, both shot with normal dose measured along the lines 504 and 508 through shot outlines of shapes 502 and 506, respectively, with the same resist threshold as indicated by the line 514. Shapes 502 and 506 are broken up to indicate rectangular shapes that are much longer than they are wide where the normal dose is used to shoot each shape on a resist with a threshold of half the normal dose. Doses below the resist threshold will not print.

In a VSB machine, the shot outlines are the shapes of eBeam projection as directed to the writer. In a multi-beam machine, the shot outlines are the shapes of the desired shapes as directed to the writer, resulting in a rasterization to pixels and eBeam projection of various doses as appropriate for the pixels used to draw the shape. To simplify comprehension, in this disclosure, dose profiles are drawn and explained as though the machines are VSB, although the embodiments may also apply to multi-beam. In a multi-beam machine, the rasterization to pixels further complicates the dose profile, and is dependent on the location of the shape relative to the pixel grid. For comprehension of the concepts of this disclosure, these additional complexities of multi-beam writing are not relevant.

For large enough shapes, the dose profile 512 reaches a plateau at the normal dose. This plateau is at the same dose even if the width of the shape 502 is larger. For smaller shapes as illustrated by shape 506, there is not enough energy to have the peak of the dose profile reach the normal dose. The shape of the dose profile 522 does not have a plateau. In addition, the dose profile 522 does not cross the resist threshold 514 at the same location as the width of the shape 506. Because there is not sufficient energy, the exposed shape on the resist will be narrower than the desired width.

Dose margins of the left edge of the shapes 502 and 506 are indicated by the edge slopes 516 and 528, respectively. Slope 528 is shallower than slope 516. The narrower the shape 506, the lower the dose profile and the shallower the slope 528 will become. Once the shape 502 is wide enough for dose profile 512 to hit the plateau, wider shapes will not change the slope 516. Shallower slopes have worse dose margin, meaning that the critical dimension (CD) that is the width of the shape is subject to more variation given a certain dose variation. The term dose margin here describes the tolerance of a pattern defined by a set of charged particle beam shots to manufacturing variations of all types including dosage related variations. A better dose margin indicates a higher tolerance. For those skilled in the art, it is generally understood that resilience to dose variation is a good proxy for many sources of manufacturing variation. To improve resilience to manufacturing variation as indicated by dose margin, one conventional method is to use a higher than normal base dose for smaller shapes, such as depicted by dose profile 532 of FIG. 5C. A base dose of more than 1.0 is used in this example where the dose amount is chosen so as to have the CD indicated by the distance between the points of dose profile 532 that cross the resist threshold 514 be the desired width of the target shape 506. The industry uses many combinations of dose adjustment and shape adjustment. FIG. 5C is one example where only dose adjustment is deployed. In this example, once the dose is calculated for shape 506, the dose margin may be measured by calculating the slope 538 of the dose profile 532 where it crosses the threshold 514. Note that edge slope 538 is better (i.e., has a steeper slope) than edge slope 528, but may still be worse than edge slope 516.

Dose margin is also important for printability of the small features because of contrast. Contrast is the difference in amount of energy applied to the resist in the immediate neighborhood interior to the exposed area versus in the immediate neighborhood exterior to the exposed area. Immediate neighborhood in semiconductor mask processing may be a few nanometers to a few tens of nanometers. Because a dose profile is a continuous function in the length scale of concern, dose margin and contrast are highly correlated to each other. Insufficient contrast will make a shape unresolvable. Reducing the minimum size of the shapes that can reliably resolve with a given resist is important to the economics of mask making.

There is another factor that influences the amount of dose that needs to be cast directly by the eBeam writer to print a shape on the surface. It is called proximity effect correction (PEC) which corrects for backscatter of electrons cast by eBeam “shots” around the area of concern. FIGS. 6A-6B show the resulting dose corresponding to the shots of FIGS. 5A-5B after PEC. In FIG. 6A, backscatter of electrons cast by shape 502 and its surrounding shots, typically within distance from a shot on the order of 10 μm, is indicated by the dashed line representing a backscatter 618. If the surrounding area is densely populated with exposures, the backscatter 618 will be higher. If the surrounding area is sparsely populated, the backscatter 618 will be lower, perhaps near zero. PEC, as generally practiced, iteratively optimizes the applied dose for a sufficiently large shape 502 so that the dose applied to shoot shape 502 causes the width of shape 502 to be printed accurately despite the added dose contributed by backscatter. The corrected dose profile 612 of the exposure (excluding backscatter) has less dose than dose profile 512. The edge slope 616 is shallower than edge slope 516. Higher amounts of backscatter received from the adjacent areas make dose margin worse. FIG. 6B shows the same PEC applied to smaller shapes, such as for SRAFs. Since PEC is normally applied the same way to all shapes of all sizes, dose profile 622 becomes even smaller in magnitude (not including the base dose coming from backscatter as shown by the horizontal dashed line for backscatter 618) as compared to dose profile 522. Edge slope 628 therefore is even shallower than edge slope 528, and substantially shallower than edge slope 616, making dose margin worse and these shapes much more susceptible to effects of manufacturing variation. FIG. 6C shows the post-PEC dose profile of the shot described in FIG. 5C where the dose was increased to meet the desired critical dimension (CD). Edge slope 638 is shallower (worse) than pre-PEC edge slope 538, but is better than the normal dose, post-PEC edge slope 628.

In some embodiments, providing sufficient dose margin includes increasing dose such that post-PEC dose is within a pre-set limit (such as 0.7 to 1.3 times the normal dose) and performing linearity correction to insure the size of the shape is correct.

Backscatter is caused by charged particles, such as electrons, that “bounce” back after colliding with the resist and materials under the resist. The effective radius of backscatter may be, for example, 10 microns—much larger than the size of a shot. Therefore, all the backscatter from nearby shots within that effective radius of a shot will add dosage at the shot's position. If not corrected for, backscatter may add more dose to the shot than the shot's intended dose, causing patterns to register wider—more so in areas of high exposure density.

FIGS. 7A-7G show an iteration sequence applied by PEC to correct dose amounts used to shoot each shape to correct for backscatter effects as known in the art. FIG. 7A illustrates an example of an outline of a rectangular shot 702. The breaks show that shot 702 may be arbitrarily long in the vertical direction. The width of the shot 702, the distance between “g” and “h”, for illustration purposes is assumed to be between 100 nm and 300 nm in this example presuming a commonly used mask production process, significantly less than the assumed backscatter range of approximately 10 m. Shot sizes of multibeam machines are typically 5-20 nm. In the case of a multibeam machine, a collection of shots combined together shoots a shape such as shot 702. Backscatter applies to a single shot in the same way as a collection of shots and PEC correction is applied in the same way. FIG. 7B illustrates an example of a dosage graph 710 illustrating dosage along the line 704 through shot outline 702 with a normal shot dosage, with nearly no backscatter. Other long-range effects are also assumed to contribute nothing to the background exposure of FIG. 7B, leading to a near-zero background exposure level. The total dosage delivered to the resist is illustrated on the y-axis, and is 1.0 times the normal dosage. Because of the near-zero background exposure, the total dosage and the shot dosage are nearly the same. Dosage graph 710 also illustrates a resist threshold 714 at half the normal dosage. The CD variation of the shape represented by dosage graph 710 in the x-direction is inversely related to the slope of the dosage curve (i.e., dose profile) 712 at x-coordinates “g” and “h” where it intersects the resist threshold 714. The edge slope 716 of dosage curve 712 at threshold 714 is illustrated as the hypotenuse of a right triangle.

The FIG. 7B condition of near-zero background exposure is not reflective of actual designs. Actual designs will typically have many other shots within the backscattering distance of shot 702. FIG. 7C illustrates an example of a dosage graph 720 of a shot with a normal dosage with a backscatter 728 resulting from a 50% exposure density. In dosage graph 720, dosage curve 722 illustrates the cross-sectional dosage of shot 702 in addition to the background exposure (backscatter 728). The edge slope 726 of the dosage curve 722 at threshold 714 is illustrated as the hypotenuse of a right triangle. The CD variation of curve 722 is greater (worse) than the CD variation of curve 712, as indicated by the shallower edge slope 726 where curve 722 intersects the resist threshold 714 beyond points “g” and “h”, compared to edge slope 716. The shallower edge slope 726 is due to the resist threshold intersecting the lower part of the dose curve where dose margin is worse due to the background exposure caused by backscatter 728. The intersection of the dosage curve 722 at the resist threshold 714 is wider than points “g” and “h” indicating that the printed CD would be larger than the desired size. The backscatter 728 “pre-exposes” the resist, so shooting dosage curve 722 with normal dosage in the presence of backscatter 728 causes the CD to print larger than desired.

FIG. 7D illustrates a new dose curve 732 after PEC. Interim dose graph 725 still shows 50% backscatter 728 but with a reduced dose curve 732, calculated such that with the current backscatter the intersection of dose curve 732 and resist threshold 714 measures exactly at “g” and “h.” This is the result of a first iteration of PEC to correct the overdosing that comes from the presence of backscatter. In this iteration, the backscatter amount is assumed to be the same as backscatter 728 because there is no way to know what the new backscatter will be after PEC is performed for all surrounding shots. PEC computation decreases the dose applied to shot 702 so that the resist threshold 714 intersects dose profile 732 at “g” and “h”. The edge slope 736 of the dosage curve 732 at threshold 714 is illustrated as the hypotenuse of a right triangle. Note that slope 736 is shallower than slope 716 as PEC makes dose margin worse.

Dose graph 730 of FIG. 7E illustrates why PEC needs multiple iterations. The PEC calculation performed as illustrated in FIG. 7D hits “g” and “h” exactly, if and only if backscatter 738 is identical to backscatter 728. But since PEC is performed for all shots, the backscatter 738 will be decreased because all shots around this shot would have PEC applied to them, resulting in each shot dose decreasing (as this shot's dose was decreased from curve 722 to curve 732). The new backscatter is indicated in FIG. 7E as backscatter 738. Backscatter 738 is lower than backscatter 728. As can be seen, the reduction in backscatter results in a smaller registered pattern size than the desired size of the original shot 702.

The second iteration of PEC corrects for this by recomputing PEC with this new (reduced) backscatter amount (backscatter 738). Now with lower backscatter, dose profile 732 needs to be enhanced with increased dose to hit targets “g” and “h” to print a shape such as shot 702 with the correct CD.

Enhancing dose for PEC on all shapes of a design as indicated in dose graph 740 of FIG. 7F results in a dose profile 742 that is higher than dosage curve 732. Subsequently, after all other shapes in the neighborhood are adjusted a higher backscatter 748 than backscatter 738 will result. The third iteration of PEC corrects for this by recomputing PEC again with this new (increased) backscatter amount. These iterations continue alternately until there is convergence within a pre-determined tolerance of the backscatter amount as indicated at dose level 758 in dose graph 750 of FIG. 7G and dose profile 752 correctly producing the desired size of original shot 702 at threshold 714. The converged dose amounts are then used to shoot the individual shapes on the mask, resulting in a backscatter corrected set of doses for all shapes as the PEC result.

FIGS. 8A-8B illustrate an example of how PEC affects isolated shapes. In FIG. 8A shapes 810 and 815 are isolated patterns in an area otherwise occupied by no other exposure. Initial dose can be calculated at 1.0 times the normal dose for both shapes. FIG. 8B shows that dosages calculated after PEC are still approximately 1.0 of the normal dose, being virtually unaffected as a result of no surrounding backscatter other than from backscatter contributed by shapes 810 and 815.

FIGS. 8C-8D illustrate an example of how PEC affects shapes in 50% exposure density areas; that is, in which 50% of the area is covered with patterns. In FIG. 8C, shapes 820, 822, 824, 826 and 828 are shown in a repeated line and space pattern where the dosed shape and the space in between are equal in width, with the line and space pattern repeated for an effective radius of 10 μm in all directions. Initial dose for each shape can be calculated at 1.0 times the normal dose. FIG. 8D shows as an example that because of surrounding backscatter from neighboring shapes, during PEC, dosage is reduced to 0.67 of the normal dose for all shapes in the repeated pattern.

FIGS. 8E-8F illustrate an example of how PEC affects shapes in high density areas. In FIG. 8E, shapes 830, 832 and 834 are shown where shape 832 is the shape of concern. Shapes 830 and 834 are large areas of exposure of width greater than an effective radius of 10 μm in width, and the pattern is extended above and below by an effective radius of 10 μm. Initial dose for each shape can be calculated at 1.0 times the normal dose. FIG. 8F shows that because of surrounding backscatter from neighboring shapes during PEC, dosage is reduced to, for example, 0.5 of the normal dose for shape 832. PEC mathematically reduces the dose of each exposure by just the right amount to make the CD equal to what the CD would have been without backscatter for a sufficiently large shape. PEC therefore effectively makes the effect of backscatter disappear. Backscatter is always a positive value. Therefore, PEC always reduces dose to compensate.

Because PEC works by “flattening” the Gaussian, the dose needed to expose the shape in an area of high backscatter is significantly less. The difference in required dose between the area with high backscatter (the shape is surrounded by high dose density) vs. an area with no backscatter (the shape is surrounded by low dose density) can be as much as 2× or more. The modified dose D_(pec) of a pixel or a shot with normal dose for the first iteration of PEC calculation is given by the following formula:

$D_{pec} = \frac{T_{emp}}{T_{emp} + {\eta \left\lbrack {{dose}\mspace{14mu} {density}} \right\rbrack}}$

At the resist threshold of 0.5 of the normal dose. T_(emp.) is the fraction of forward scatter at the resist threshold and eta(η) is the normalization constant. With T_(emp) of 0.5, an eta(η) of 0.5 and an exposure density of 100%. D_(pec) is calculated to be 0.5. If an SRAF is assigned to be shot with twice the normal dose (2.0 times) but is in an area of high density with high backscatter, the pixels or shots will end up with approximately 1.0 times the normal dose as 0.5*(2.0)=1.0 after the first iteration of PEC calculation.

This is because the area is largely exposed with energy from backscatter. So only a fraction of the energy from this pixel or shot is needed to cast enough energy to reach the threshold for exposing the resist.

Areas with near-zero backscatter take the most eBeam dose per shot. Therefore, in a constant write time multi-beam writer, the write time of the entire machine is paced by the writing of those isolated patterns with the highest enhanced dose, typically for narrow shapes such as for SRAFs. Typical test masks have patterns in high density areas mixed with patterns in low density areas. Typical production masks have much less variation. Some masks have patterns that are all dense (for example 70% exposure density on the average). Other masks have patterns that are all sparse (for example, 25% exposure density on the average). But as many production masks combine some test patterns in them, low variation cannot be assured. In any case, multi-beam writing speed, particularly for constant write time writers, is dictated by the pixel that combines a high enhanced dose in an environment that has less backscatter cast. To a lesser degree, but still significantly, the writing speed of variable write time writers such as VSB writers and possibly multi-beam writers are paced by the shot that combines a high enhanced dose in an environment that has less backscatter.

Artificial Background Dose

In some embodiments, an artificial background dose is introduced in areas of otherwise low backscatter to reduce pixel or shot dose and hence reduce overall write time. The pixels or shots will have lower dose after PEC as a result, decreasing the maximum of the pixel or shot doses for a mask or a section of the mask, increasing the stage moving speed, and thereby reducing the overall write time significantly.

FIGS. 9A-B illustrate how introducing artificial background dose in accordance with some embodiments can mimic a 50% density similar to FIGS. 8C and 8D. FIG. 9A shows similar isolated shapes 910 and 915 as FIG. 8A but with an added artificial background dose in the form of a shape 913. Initial dosage is set at 1.0 times the normal dose for shapes 910 and 915 as before and an artificial background dose that is 0.30 of the normal dose for shape 913 in this example. It is important to note that a dosage applied to this new shape 913 is below the threshold to print. FIG. 9B shows similar dosage reduction at 0.67 of the normal dose after PEC as FIG. 8D, reducing overall dosage required to print previously isolated shapes 910 and 915. In some embodiments shape 913 is also reduced to 0.20 of the normal dose. In this simplified example, shape 913 is assumed to extend beyond the backscatter radius away from shapes 910 and 915. In most situations, the shape 913 will be much reduced in size so as to add the artificial background dose only in the area immediately surrounding shapes 910 and 915. Other such artificial background dose for other shapes surrounding shapes 910, 913, and 915 will contribute actual backscatter to these shapes. In the present embodiments, all such energy contributions are computed using PEC when the actual post-PEC dose of shapes 910 and 915 are computed. In some embodiments, the dose of shape 913 is not modified by all iterations of PEC. In some embodiments, the dose of shape 913 is modified through all iterations of PEC.

Artificial background dose can be added to areas where backscatter is low enough where post-PEC dose margins are sufficiently better than “good enough” according to some parameter set by practice. FIGS. 10A-10F illustrate a few examples of artificial background dose, where the added artificial background dose is in the form of an additional pattern (patterns with hashed fill lines) that will be shot in combination with the desired pattern. The artificial background dose is a sub-threshold exposure; that is, a dosage lower than the resist threshold required to print. FIG. 10A shows how artificial background dose shape 1001 can be cast over an area containing a desired pattern shape 1000 to be printed on a surface, completely covering the pattern in the area. FIG. 10B shows artificial background dose shape 1002 in the area except where the desired pattern shape 1000 already exists, so as not to cover the pattern. FIG. 10C shows artificial background dose shape 1003 in the area that surrounds the desired pattern shape 1000 with some margin, for example up to 3 sigma away from the pattern's edge. For large enough patterns as in a pattern shape 1010 in FIG. 10D, artificial background dose shapes 1011 and 1012 are applied only beyond a pre-determined distance from an edge of the pattern shape 1010 to be printed on a surface. Creating a margin around a feature, for example an edge, a line end or an SRAF, artificial background dose applied in this way in some cases may be better than just increasing background exposure everywhere. Artificial background dose can alternatively be added anywhere to the area as shown for example, in each of FIGS. 10E and 10F, with artificial background dose shapes 1004 and 1005 partially covering the desired pattern shape 1000, respectively.

In some embodiments a pre-determined artificial background dose, such as in the range of 20% to 30%, is defined and applied everywhere. A minimum target backscatter amount, or pre-determined threshold, for example 30%, is defined. In some embodiments, where there is not naturally sufficient backscatter for PEC to decrease dose, surrounding dose is increased by adding artificial background dose to meet the minimum backscatter amount. In some embodiments, the additional backscatter contributed by the artificial background dose may or may not be taken into account in the amount of artificial background dose to add by pre-computing the additional backscatter as contributed by the artificial background dose. The embodiments described herein are examples and other variations of adding artificial background dose are possible. In some embodiments, the minimum backscatter amount will have built-in margin to account for the additional backscatter emanating from the artificial background dose. Since backscatter amounts are mathematically linear in behavior, the amount of backscatter added by the artificial background dose can be computed independently of the doses of the shots in any given region. In some embodiments, the total mask area will be subdivided into partitions of some size or sizes, and the artificial background dose is determined for each partition, with each of the partitions having one artificial background dose amount within the partition, but different partitions having potentially different artificial background dose amounts. Typically. PEC is computed on a coarse grid, such as a 50 nm grid, or 300 nm grid. For each grid or partition, the PEC adjustment is computed. In some implementations, the PEC adjustment for any location within a partition is interpolated based on the computed PEC adjustments for adjacent partitions. In some embodiments, the computing of the artificial background dose amount is done on the same grid as the grid used for PEC. In such an implementation, the received backscatter amount in each PEC grid is compared to the specified minimum target backscatter amount to determine the artificial background dose amount to provide for the area that the PEC grid covers. In some embodiments the artificial background dose for any location within an individual partition is interpolated across the partition, such as based on the artificial background doses for adjacent partitions. The ensuing PEC step will decrease the dose of the shot/pixel in question, decreasing the write time for that shot/pixel. Doing this for all shots/pixels on the mask or a section of the mask decreases the dose and hence the write time for that section of the mask. The ensuing PEC step accounts for the addition of the artificial background dose and any additional backscatter contributed by artificial background dose. PEC adjusts the shot dose of all shots on the mask to adjust all CDs to hit the target in exactly the same way PEC has always worked for natural backscatter. Dose margins of adjusted shots are worse than prior to the addition of the artificial background dose. But the user adjusted parameter for minimum backscatter allows the dose margins to stay within acceptable dose margins as determined for a particular mask process.

With conventional VSB machines, casting a dose of any kind (however small in dose) requires a separate shot and blanking time separating the shots. Since blanking time is typically about the same amount of time as the exposure time at normal dose, at normal dose, a reasonable first-order approximation of a shot time might be considered to take 2 time units. In this approximation, a shot of 10% dose would take 1.1 time units. Since write time is of principal importance in optimizing both cost and yield of masks, and since complex leading edge masks are already seen to be taking too long to write, it is not commercially feasible to add artificial background dose everywhere there were otherwise no shots. Nevertheless, since the mask stage, which is typically variable speed, is heavy in a VSB mask writer, the mask stage can only change speeds gradually, therefore reducing peak dose density can help reduce write time for VSB machines.

Particularly for VSB machines, some embodiments of the present disclosure include purposefully leaking some eBeam energy, producing artificial background dose, during blanking time. The exact location of where the leaked eBeam is cast need not be precisely controlled. Since backscatter is a large-scale effect in the 10 μm radius range, nm-level control of location is not important. The amount of leakage and the period of leakage during the blanking time can be precisely calculated. Such calculation can compute the path that the eBeam is travelling and avoid casting the leakage close to (i.e., within the combined forward blur of) any pattern edge that needs precise control.

Surface writing for the most advanced technology nodes typically involves multiple passes of charged particle beam writing, a process called multi-pass exposure, whereby the given shape on the reticle is written and overwritten. Typically, two to four passes are used to write a reticle to average out precision errors in the charged particle beam writer, allowing the creation of more accurate photomasks. Also typically, the list of shots, including the dosages, is the same for every pass. In one variation of multi-pass exposure, the lists of shots may vary among exposure passes, but the union of the shots in any exposure pass covers the same area. Multi-pass writing can reduce over-heating of the resist coating the surface. Multi-pass writing also averages out random errors of the charged particle beam writer. Multi-pass writing using different shot lists for different exposure passes can also reduce the effects of certain systemic errors in the writing process. In some embodiments, in VSB and multi-pass writing, only one or some of the writing passes cast the artificial background dose. In other words, in some embodiments the original set of exposure information comprises information for multiple exposure passes, and wherein the artificial background dose is only added in an exposure pass. Since precision is not important for artificial background dose, this is sufficient, and it saves writing time by not affecting all passes. The other passes have reduced peak dose of a pixel or a reduced peak dose density of an area without the additional write time required for the artificial background dose, such as in the embodiment depicted in FIG. 10A.

In some embodiments, a relatively isolated pattern is purposefully surrounded by artificial background dose resulting in increased backscatter. PEC, the correction for backscatter, is accomplished by reducing the pixel or shot dosage—less reduction where the exposure density is low, and more reduction where the exposure density is high. However, reducing dose worsens dose margin.

An acceptable dose margin can be determined by the amount of size variation caused by the reduction in dose. In one embodiment an isolated pattern exposed with normal dose can be shot using a larger pattern and a reduced dose to an acceptable level without adding artificial background dose.

In exposing, for example, a repeated pattern on a surface using charged particle beam lithography, the size of each pattern instance, as measured on the final manufactured surface, will be slightly different, due to manufacturing variations. The amount of the size variation is an essential manufacturing optimization criterion. Too much variation, particularly for the minimum sized features, may result in that shape not being printed at all, causing the resulting circuit to malfunction. Manufacturing variations, such as line-edge roughness and corner rounding, will also be present in the actual patterns on a surface. In addition, more size variation translates to more variation in circuit performance, leading to higher design margins being required, making it increasingly difficult to design faster, lower-power integrated circuits. This variation is referred to as critical dimension (CD) variation. A low CD variation, in particular a uniformly low CD variation across all shapes across the mask, is desirable, and indicates that manufacturing variations will produce relatively small size variations on the final manufactured surface. In the smaller scale, the effects of a high CD variation may be observed as line edge roughness (LER). LER is caused by each part of a line edge being slightly differently manufactured, leading to some waviness in a line that is intended to have a straight edge. CD variation is inversely related to the slope of the dosage curve at the resist threshold, which is called edge slope. Therefore, edge slope and its inverse, dose margin, is a critical optimization factor for particle beam writing of surfaces. In this disclosure, edge slope and dose margin are terms that are used interchangeably.

In some embodiments, methods include suggesting an appropriate amount of artificial background dose through the use of an edge slope that meets a target level; that is, an edge slope that is “good enough.” Since resilience to manufacturing variation is a statistical notion, the sense of a “good enough” edge slope is not an exact expression of a strict inequality. In some embodiments of the present methods, the amount of artificial background dose is determined in which the edge slopes are above a “good enough” level. For example, a particular mask manufacturing process may be tuned to produce reliable manufacturing results for 100 nm×2 μm lines being written in a 75% exposure density area, producing a larger amount of backscatter, therefore having the least amount of shot/pixel dose post-PEC, and therefore having a relatively shallow edge slope. In some embodiments, the edge slope of that line post-PEC is designated as “good enough.” While there will be other shapes, such as a 40 nm×200 nm space being written in a 75% density area, where edge slope is worse, the mask manufacturing process may determine that the edge slope there is not “good enough” but is still manufacturable in the overall tradeoff of economics, time, and manufacturing reliability. The function of the “good enough” edge slope for the present embodiments is to designate that being even better than “good enough” is taking too much time to cast that dose as compared to the incremental benefit of resilience to manufacturing variation. Decreasing edge slope to a less than optimal level—that is, below a target level—is counter-intuitive since the conventional teaching is to maximize edge slope.

In some embodiments, the artificial background dose amount is computed automatically. In one embodiment, artificial background dose can be computed to achieve an acceptable level of contrast (a reduction in contrast). In another embodiment, artificial background dose can be computed to achieve a dose margin with an edge slope above a target minimum. The minimum acceptable edge slope can be determined by calculating an edge slope at a pre-determined edge location of a pre-determined pattern in a pre-determined backscatter area.

In some embodiments, artificial background dose is added before PEC to reduce write time, by decreasing dosage during PEC where the edge slope with the decreased dosage may be below a target level. In some embodiments, a target or “good enough” level may be calculated by simulating the edge slope of a feature that is known in the manufacturing process to be working sufficiently well to be used for production purposes. For example, for leading edge photomask manufacturing, a repeating pattern of 100 nm wide wires separated by 100 nm wide spaces is made to be stable, when exposed with a normal dose before PEC. A simulation of the edge slope for a 100 nm wide line in the context of a 100 nm line and space pattern may be considered a dose margin that is “good enough.” For purposes of calculating artificial background dose, a 100 nm line-and-space pattern has a 50% exposure density in the surrounding area. A natural backscatter resulting from the 50% exposure density is calculated as a minimum backscatter amount. The sum of natural backscatter already present in an area plus an amount of artificial background dose is evenly distributed so as to contribute an overall background exposure up to the minimum backscatter that is uniform throughout the mask. Although a 50% exposure density may not produce the worst acceptable dose margin post-PEC, it may be declared as a good practical target to achieve for the purposes of computing the amount of minimum acceptable dose from which artificial background dose amount is computed.

FIG. 11 is a conceptual flow diagram 1100 for preparing a surface such as a reticle or other surface, using charged particle beam lithography, as known in the art. In a first step 1102, a physical design, such as a physical design of an integrated circuit, is created. This can include determining the logic gates, transistors, metal layers, and other items that are required to be found in a physical design such as the physical design of an integrated circuit. Next, in a step 1104, optical proximity correction (OPC) is determined for the physical design of step 1102 or on a portion of the physical design desired on the wafer to create a mask design 1106. OPC computes the mask shapes needed to best produce the desired wafer shapes across manufacturing variation. OPC alters the physical design to compensate for distortions caused by effects such as optical diffraction and the optical interaction of features with proximate features producing the mask design 1106. In a step 1108, a mask data preparation (MDP) operation which may include a fracturing operation, a shot placement operation, a dose assignment operation, or a shot sequence optimization. In some embodiments that are for multi-beam mask writing. MDP step 1108 may include generating a plurality of multi-beam shots, each multi-beam shot comprising one or more beamlets, where dosage areas are determined and dosages assigned to beamlets in each dosage area. In some embodiments, beamlet dosages may vary within a dosage area.

A proximity effect correction (PEC) refinement is performed in step 1118, in which dosages are adjusted to account for backscatter, fogging, and loading effects, creating an exposure information in step 1120 with adjusted dosages. The adjusted dosages in exposure information of step 1120 are used to generate a surface in a mask writing step 1122, which uses a charged particle beam writer such as an electron beam writer system. Depending on the type of charged particle beam writer being used, the PEC refinement 1118 may be performed by the charged particle beam writer. Mask writing step 1122 may comprise a single exposure pass or multiple exposure passes. The electron beam writer system projects a beam of electrons through a stencil or aperture plate onto a surface to form a mask image 1124 comprising patterns on the surface. The completed surface, such as a reticle, may then be used in an optical lithography machine, which is shown in a step 1126.

FIG. 13 illustrates a flow 1300 representing a method for exposing a pattern in an area on a surface, in which artificial background dose is calculated and applied, in accordance with some embodiments. In step 1305 an original set of exposure information for a pattern is input. In some embodiments, the original set of exposure information is a collection of pixels and their dosages. In another embodiment, the original set of exposure information is a set of shapes potentially including curvilinear or entirely non-polygonal descriptions (like circles or splines). In yet another embodiment the original set of exposure information is a set of shots with pre-PEC dose assigned or implied (e.g., VSB) or a set of shapes with pre-PEC dose assigned or implied (e.g., multi-beam writing). In general, the input in step 1305 is anything else that describes shapes or doses.

A backscatter is calculated in step 1310, based on the original set of exposure information. In one embodiment, the calculation of backscatter in step 1310 is an initial determination for PEC which creates an initial map of backscatter. PEC is an iterative process where dose is adjusted to print the desired size in the presence of backscatter. The initial map of backscatter from the initial PEC determination is a good relative indication of higher and lower dose density areas. In some embodiments, areas where the calculated backscatter is below a pre-determined threshold are identified in step 1312.

Calculations made in step 1314 determine an artificial background dose, where the artificial background dose comprises additional exposure information. In some embodiments, step 1314 is performed in an area with the calculated backscatter below the pre-determined threshold as determined in step 1312. In some embodiments, step 1314 adds the artificial background dose only where the calculated backscatter is below the pre-determined threshold, that is the artificial background dose is the difference between the pre-determined threshold and the calculated backscatter. In some embodiments, in step 1314 the dose margin or edge slope is calculated for a desired pattern in the area and the artificial background dose is determined to maintain “good enough” edge slope or contrast for the desired pattern in the area. In some embodiments, step 1314 adds the artificial background dose to maintain “good enough” edge slope for the pattern in the area that meets a certain criteria, such as minimum subject size for a “good enough” edge slope. For example, smaller size shapes for SRAFs may be exempt from the “good enough” edge slope. As another example, smaller size shapes for SRAFs may have a different “good enough” edge slope to fulfill in determining the artificial background dose to be added. In some embodiments, these calculations can result in a creation of an artificial background dose comprising additional patterns with sub-threshold exposure such that the additional patterns will not print. In some embodiments, the calculation and the creation of additional patterns occur after MDP step 1108 of flow 1100. FIG. 11, where the additional patterns geometrically overlap the desired pattern in the mask design 1106 of flow 1100, FIG. 11. A modified set of exposure information in step 1316 containing the original set of exposure information combined with the additional exposure information (i.e., additional patterns) may be read by the proximity effect correction (PEC) refinement step 1118 of flow 1100, FIG. 11, producing an exposure information in step 1120 that includes the artificial background dose and may also include a backscatter arising from artificial background dose. In some embodiments, the modified set of exposure information reduces overall write time compared to the original set of exposure information. In some embodiments, the modified set of exposure information is refined by PEC resulting in adjusted dosages of the modified set of exposure information. The exposure information is then used to expose the surface in 1124. FIG. 11. In some embodiments, pixel or shot dose is modified to add the artificial background dose. In some embodiments, pixels or shots cast artificial background dose in otherwise empty areas (pixels that start out at zero dose) with the amount of dose relatively similar for pixels, for example in a 3×3 or greater number of adjacent pixels. In some embodiments, some or all of steps 1310, 1312, 1314 and 1316 of FIG. 13 followed by steps 1118 and 1120 of FIG. 11 are performed simultaneously with mask writing step 1122 of flow 1100. FIG. 11, with inline processing to perform data manipulation while the mask is being exposed. That is, in some embodiments the mask exposure is performed inline with one or more steps selected from the group consisting of calculating the backscatter, determining the area where the calculated backscatter is below a pre-determined threshold, determining the artificial background dose, and creating the modified set of exposure information.

The mask data preparation, calculation of artificial background dose and proximity effect correction described in this disclosure may be implemented using general-purpose computers using Central Processing Units (CPU) with appropriate computer software as computation devices. Due to the large amount of calculations required, multiple computers or processor cores of a CPU may also be used in parallel. In one embodiment, the computations may be subdivided into a plurality of 2-dimensional geometric regions for one or more computation-intensive steps in the flow, to support parallel processing. In another embodiment, a special-purpose hardware device, either used singly or in multiples, may be used to perform the computations of one or more steps with greater speed than using general-purpose computers or processor cores. Specialty computing hardware devices or processors may include, for example, field-programmable gate arrays (FPGA), application-specific integrated circuits (ASIC), or digital signal processor (DSP) chips. In one embodiment, the special-purpose hardware device may be a graphics processing unit (GPU). In another embodiment, the optimization and calculation processes described in this disclosure may include iterative processes of revising and recalculating possible solutions, so as to minimize the total charged particle beam writing time, or some other parameter. In yet another embodiment, the processes may be deterministic computations without iteration.

FIG. 12 illustrates an example of a computing hardware device 1200 that may be used to perform the calculations described in this disclosure. Computing hardware device 1200 comprises a central processing unit (CPU) 1202, with attached main memory 1204. The CPU may comprise, for example, eight processing cores, thereby enhancing performance of any parts of the computer software that are multi-threaded. The size of main memory 1204 may be, for example, 64 G-bytes. The CPU 1202 is connected to a Peripheral Component Interconnect Express (PCIe) bus 1220. A graphics processing unit (GPU) 1214 is also connected to the PCIe bus. In computing hardware device 1200 the GPU 1214 may or may not be connected to a graphics output device such as a video monitor. If not connected to a graphics output device, GPU 1214 may be used purely as a high-speed parallel computation engine. The computing software may obtain significantly-higher performance by using the GPU for a portion of the calculations, compared to using CPU 1202 for all the calculations. The CPU 1202 communicates with the GPU 1214 via PCIe bus 1220. In other embodiments (not illustrated) GPU 1214 may be integrated with CPU 1202, rather than being connected to PCIe bus 1220. Disk controller 1208 may also be attached to the PCIe bus, with, for example, two disks 1210 connected to disk controller 1208. Finally, a local area network (LAN) controller 1212 may also be attached to the PCIe bus, and provides Gigabit Ethernet (GbE) connectivity to other computers. In some embodiments, the computer software and/or the design data are stored on disks 1210. In other embodiments, either the computer programs or the design data or both the computer programs and the design data may be accessed from other computers or file serving hardware via the GbE Ethernet.

While the specification has been described in detail with respect to specific embodiments, it will be appreciated that those skilled in the art, upon attaining an understanding of the foregoing, may readily conceive of alterations to, variations of, and equivalents to these embodiments. These and other modifications and variations to the present methods for mask data preparation, and proximity effect correction may be practiced by those of ordinary skill in the art, without departing from the scope of the present subject matter, which is more particularly set forth in the appended claims. Furthermore, those of ordinary skill in the art will appreciate that the foregoing description is by way of example only, and is not intended to be limiting. Steps can be added to, taken from or modified from the steps in this specification without deviating from the scope of the invention. In general, any flowcharts presented are only intended to indicate one possible sequence of basic operations to achieve a function, and many variations are possible. Thus, it is intended that the present subject matter covers such modifications and variations as come within the scope of the appended claims and their equivalents. 

1. A method for exposing a pattern in an area on a surface using charged particle beam lithography, the method comprising: inputting an original set of exposure information for the area; calculating a backscatter for the area, based on the original set of exposure information; and determining an artificial background dose for the area, wherein the artificial background dose comprises additional exposure information and wherein the additional exposure information is combined with the original set of exposure information to create a modified set of exposure information.
 2. The method of claim 1, wherein the modified set of exposure information reduces overall write time compared to the original set of exposure information.
 3. The method of claim 1, wherein the modified set of exposure information is refined by PEC resulting in adjusted dosages of the modified set of exposure information.
 4. The method of claim 1, wherein the artificial background dose comprises an additional pattern with a sub-threshold exposure.
 5. The method of claim 1, wherein the artificial background dose is applied only beyond a pre-determined distance from an edge of the pattern on the surface.
 6. The method of claim 1, wherein the original set of exposure information comprises information for multiple exposure passes, and wherein the artificial background dose is only added in an exposure pass.
 7. The method of claim 1, wherein in the area for which the calculated backscatter is less than a pre-determined threshold, the artificial background dose is the difference between the pre-determined threshold and the calculated backscatter.
 8. The method of claim 1, wherein the area is subdivided into partitions, wherein the artificial background dose is determined for each partition.
 9. The method of claim 8, wherein an artificial background dose for any location within an individual partition is interpolated across the partition.
 10. The method of claim 9, wherein the interpolation is based on the artificial background doses for adjacent partitions.
 11. The method of claim 1, further comprising calculating an edge slope for the pattern to be exposed.
 12. The method of claim 11, wherein the artificial background dose is determined to achieve an edge slope of the pattern to be exposed above a target minimum, wherein the target minimum is determined by calculating the edge slope at a pre-determined edge location of a pre-determined pattern in a pre-determined backscatter area.
 13. The method of claim 1, wherein a mask exposure is performed inline with one or more steps selected from the group consisting of calculating the backscatter, determining the area where the calculated backscatter is below a pre-determined threshold, determining the artificial background dose, and creating the modified set of exposure information.
 14. The method of claim 1, further comprising exposing the surface with the modified set of exposure information.
 15. A system for exposing a pattern in an area on a surface using a charged particle beam lithography, the system comprising: a device configured to input an original set of exposure information for the area; a device configured to calculate a backscatter for the area of the pattern, based on the exposure information; and a device configured to determine an artificial background dose for the area, wherein the artificial background dose comprises additional exposure information and wherein the additional exposure information is combined with the original set of exposure information to create a modified set of exposure information.
 16. The system of claim 15, wherein the modified set of exposure information reduces overall write time compared to the original set of exposure information.
 17. The system of claim 15, wherein the modified set of exposure information is refined by PEC resulting in adjusted dosages of the modified set of exposure information.
 18. The system of claim 15, wherein the artificial background dose comprises an additional pattern with a sub-threshold exposure. 